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[Quenching of the luminescence of phosphorescent bacteria as a test for assessing the toxicity of the phenol components of sewage].

The object of this work was to estimate whether the luminescence of luminescent bacteria could be used as a biological test for assessment of the toxicity of phenol compounds in sewage. The toxicity of phenol compounds for luminescent bacteria was compared in terms of three indices: the quenching of luminescence, the inhibition of dehydrogenase activity and the ability to grow. Among the three indices, the quenching of luminescence was characterized by the highest sensitivity and the most rapid response.

Cell Division↗

Tryptophan luminescence as a probe of enzyme conformation along the O-acetylserine sulfhydrylase reaction pathway.

O-Acetylserine sulfhydrylase A (OASS-A) is a pyridoxal 5'-phosphate- (PLP-) dependent enzyme that catalyzes the last step in the synthesis of L-cysteine, the beta-replacement of acetate in O-acetyl-L-serine (OAS) by sulfide. The phosphorescence properties of the two tryptophans of wild-type OASS-A, W51 and W162, and of W162 in the W51Y mutant protein have been characterized over the temperature range 170-273 K. In glasses at 170 K, the apoenzyme exhibits a phosphorescence spectrum which is the superposition of two spectra with well-resolved 0,0 vibronic bands centered at 405 and 410 nm, the blue lambda max suggesting that one of the two Trp residues in OASS-A is in a polar pocket, while the other is in a relatively hydrophobic pocket. The presence of PLP in the OASS-A holoenzyme reduces the intrinsic fluorescence by 40-45%, but the spectrum is unaltered except for the appearance of the internal Schiff base ketoenamine fluorescence band centered at 484 nm. The phosphorescence is strongly quenched by PLP, with about 70% reduction in intensity and lifetime. Further, the phosphorescence spectrum of the holoprotein exhibits a single and narrow 0,0 vibronic band centered at 405 nm and a broad band in the 450-550-nm range resulting from delayed fluorescence of the ketoenamine tautomer of the internal Schiff base, sensitized by triplet-singlet energy transfer from tryptophan to the ketoenamine tautomer of PLP. Comparison with data obtained for the W51Y mutant strongly suggests that the 405-nm phosphorescence band derives from W162, and that W51 in the wild type is entirely quenched either by singlet or triplet energy transfer to PLP or by some local group in the protein. From the rate of energy transfer, the separation between W162 and PLP is estimated to be about 25 A. Substrates other than OAS affect only the intensity of the coenzyme fluorescence band (484 nm) and the intensity of delayed fluorescence relative to that of phosphorescence, effects that are attributable to changes in fluorescence quantum yield of the ketoenamine chromophore. Addition of OAS, on the other hand, leads to a splitting of the 0,0 vibronic band in the phosphorescence spectrum of W162, yielding poorly resolved peaks at 406 and 408.5 nm, indicating thereby a change in the environment of the tryptophan residue and therefore in the conformation of the macromolecule as the internal Schiff base is converted to the alpha-aminoacrylate Schiff base. In buffer at 273 K, both the fluorescence and phosphorescence spectra relax to longer wavelengths and the phosphorescence lifetime is reduced to a few milliseconds, all indications that W162 is in a flexible region of the macromolecule, probably in close proximity to the aqueous interface. The phosphorescence lifetime in fluid medium reveals conformational heterogeneity in OASS-A and unveils important structure modulating effects of cofactor, substrates, and pH. Binding of PLP to the apoprotein increases the rigidity of the polypeptide in the region of W162 (in agreement with the greater thermal stability of the holoprotein), while OAS and L-serine have an opposite effect. Increasing the pH from 6.5 to 9 results in a 1.7-fold increase in tau av and a change in the relative amplitudes of the two lifetime components. Since the phosphorescence originates from a single tryptophan residue, the two tau components reflect distinct conformations of the subunit. In this case the conformational equilibrium (slow on the phosphorescence time scale) is governed by one or more groups in the protein with a pK around 8.

Cold Temperature↗

Spectroscopic characterization of the 4-hydroxy catechol estrogen quinones-derived GSH and N-acetylated Cys conjugates.

Estrogens, including the natural hormones estrone (E(1)) and estradiol (E(2)), are thought to be involved in tumor induction. Specifically, catechol estrogen quinones (CEQs) derived from the catechol estrogens 4-hydroxyestrone (4-OHE(1)) and 4-hydroxyestradiol (4-OHE(2)) react with DNA and form DNA adducts (Cavalieri, E. L., et al. (1997) Proc. Natl Acad. Sci. U.S.A. 94, 10037). CEQs are also conjugated with GSH, a reaction that prevents damage to DNA, providing biomarkers of exposure to CEQs. Current detection limits for these analytes by HPLC with multichannel electrochemical detection are in the picomole range (Devanesan, P., et al. (2001) Carcinogenesis 22, 489). To improve the detection limit of CEQ-derived conjugates, spectrophotometric monitoring was investigated. Fluorescence and/or phosphorescence spectra of the 4-OHE(1), 4-OHE(2), Cys, N-acetylcysteine (NAcCys), 4-OHE(1)-2-SG, and 4-OHE(2)-2-SG conjugates and their decomposition products 4-OHE(1)-2-NAcCys and 4-OHE(2)-2-NAcCys were obtained at 300 and 77 K. It is shown that (i) 4-OHE(1)- and 4-OHE(2)-derived SG and NAcCys conjugates are weakly fluorescent at 300 K (with the emission maximum at 332 nm) but strongly phosphorescent at 77 K; (ii) Cys and NAcCys exhibit fluorescence and phosphorescence only at 77 K; and (iii) 4-OHE(1) and 4-OHE(2) are weakly fluorescent at 300 and 77 K and not phosphorescent. The phosphorescence spectra of SG and NAcCys conjugates are characterized by a weak origin band at approximately 383 nm and two intense vibronic bands at 407 and 425 nm. After they are cooled from 300 to 77 K, the total luminescence intensity of SG and NAcCys conjugates increases by a factor of approximately 150 predominantly due to phosphorescence enhancement. Theoretical calculations revealed, in agreement with the experimental data, that the lowest singlet (S(1)) and triplet (T(1)) states of 4-OHE(2)-2-NAcCys are of n,pi* and pi,pi* character, respectively, leading to a large intersystem crossing yield and strong phosphorescence. The limit of detection (LOD) for CEQ-derived conjugates, based on phosphorescence measurements, is in the low femtomole range. The concentration LOD is approximately 10(-9) M. Therefore, we propose that capillary electrophoresis interfaced with low temperature phosphorescence detection can be used to test for human exposure to CEQs by analyzing urine.

Acetylcysteine↗

Imaging oxygen pressure in the retina of the mouse eye.

The phosphorescence lifetime imaging system previously used to image oxygen in the retina of the cat eye was modified to allow imaging of phosphorescence lifetimes in the much smaller mouse eye. Following the lead of Shonat and coworkers, a frequency domain approach was used in which the excitation light source was modulated in a 50% on: 50% off square wave while the gate of the intensified CCD camera was similarly modulated but delayed with respect to the excitation. These were analyzed by fitting the intensity at each pixel to a sinusoid. The phase of the phosphorescence relative to the excitation was determined and from the phase shift and frequency, the phosphorescence lifetime was calculated. The Stern-Volmer relationship was then used to calculate the oxygen pressure at each pixel of the image array. High resolution maps of phosphorescence lifetime and oxygen pressure in the retina of the mouse eye have been attained. The retinal veins draining into the optic head appear as large, highly phosphorescent vessels against a lower phosphorescence background with a network of smaller vessels. The oxygen pressure in the retinal veins is typically from 20 to 30 mm Hg while the background has somewhat higher oxygen pressures. Experiments are underway to resolve the oxygen in the choroid from that in the retina. The arteries on the retinal surface can be observed, but their small diameter, relatively high oxygen pressures (> 90 mm Hg), and surrounding tissue with much lower oxygen pressures, makes accurate determination of the oxygen pressure a challenge.

Animals↗

Noninvasive imaging of the distribution in oxygen in tissue in vivo using near-infrared phosphors.

A newly developed water-soluble phosphor suitable for measuring oxygen pressure in the blood (Green 2W) was used for noninvasive, in vivo imaging of oxygen distribution in the vascular systems of mice. Oxygen quenches the phosphorescence of Green 2W, measured in the presence of 2% albumin, according to the Stern-volmer relationship. This oxygen-dependent quenching of phosphorescence has been used to obtain digital maps of the oxygen distribution in the tissue vasculature. EMT-6 mammary carcinoma tumors were grown by injecting 1 x 10(6) cells in 0.1-ml carrier into the subcutaneous space over the muscle on the hindquarter. When the tumors were approximately 8 mm in diameter, 300 micrograms of phosphorescence probe (Green 2W; absorption maximum 636 nm) was injected into the tail vein. The mice were immobilized with intraperotoneal Ketamine (133 mg/kg) and Xylazine (10 mg/kg) and illuminated with flashes (< 4-microseconds t1/2) of light of 630 +/- 12 nm. The emitted phosphorescence (790-nm maximum) was imaged an intensified CCD camera. Images were collected beginning at 30, 50, 80, 120, 180, 240, 420, and 2500 microseconds after the flash and used to calculate digital maps of the phosphorescence lifetimes and oxygen pressure. Both the illumination light and the phosphorescence were in the near-infrared region of the spectrum, where tissue has greatly decreased absorbance. The light therefore readily passed through the skin and centimeter thicknesses of tissue. The oxygen maps could be obtained by illuminating from the side of the mouse opposite the camera (and tumor). The tumors were readily observed as regions with oxygen pressures substantially below those of the surrounding tissue. Thus, phosphorescence measurements can noninvasively detect volumes of tissue with below-normal oxygen pressure in the presence of much larger volumes of tissue with normal oxygen pressures. In addition, tissue oxygen pressures can be monitored in real time, even through centimeter thicknesses of tissue.

Animals↗